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t-CH3HC=CHCl |
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Chlorine |
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Nuclear
Quadrupole Coupling Constants |
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in trans-1-Chloropropene |
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Calculation of the chlorine
nqcc's in trans-1-chloropropene was made on a molecular
structure derived ab initio, as described
below. These are compared with the experimental nqcc's of Beaudet [1]
in Table 1. Structure parameters are given
in Z-matrix format in Table 2. |
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In Table 1, RMS is the root mean square difference
between calculated and experimental diagonal nqcc's (percentage of the
average of the magnitudes of the experimental nqcc's). RSD is the
calibration residual standard deviation for the B1LYP/TZV(3df,2p) model
for calculation of the chlorine nqcc's. |
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Subscripts a,b,c refer to the
principal axes of the inertia tensor; x,y,z to the principal axes
of the nqcc tensor. The nqcc y-axis is chosen coincident with the
inertia c-axis, these are perpendicular to the molecular symmetry plane.
Ø (degrees) is the angle between its subscripted
parameters. ETA = (Xxx - Xyy)/Xzz. |
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Table 1. Chlorine
nqcc's in t-1-Chloropropene, conformer I (see below) (MHz). |
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Calc. |
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Expt. [1] |
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35Cl |
Xaa |
- |
60.67 |
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60.3 |
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Xbb |
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28.88 |
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28.7 |
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Xcc |
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31.79 |
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31.6 |
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|Xab| |
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31.13 |
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RMS |
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0.3 (0.75 %) |
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RSD |
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0.49 (1.1 %) |
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Xxx |
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38.63 |
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Xyy |
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31.79 |
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Xzz |
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70.43 |
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ETA |
- |
0.097 |
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Øz,a |
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17.40 |
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Øa,CCl |
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17.20 |
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Øz,CCl |
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0.20 |
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37Cl |
Xaa |
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47.86 |
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Xbb |
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22.80 |
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Xcc |
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25.06 |
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|Xab| |
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24.47 |
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RSD |
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0.44 (1.1 %) |
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Cl is trans with respect
to CH3. Within the framework of Cs symmetry,
one methyl H lies in the plane of symmetry, one above and one below the plane.
With respect to the C(1)C(2)C(3) backbone, the in-plane H may be trans
(conformer I) or cis (conformer II) with Cl. Calculation was made on
both structures. At the B1LYP/TZV(3df,2p) level of theory, EI
< EII by 2.0 kcal/mol. The calculated nqcc's shown
in Table 1 are for conformer I, for which the RMS difference between calculated
and experimental nqcc's is 0.3 MHz. For conformer II, calculated Xaa,
Xbb, and Xcc are respectively -60.76, 28.95,
and 31.80 MHz. The RMS difference is, as above, 0.3 MHz. |
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Molecular Structure |
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The molecular structure
was optimized at the MP2/6-311+G(d,p) level of theory assuming
Cs symmetry. The optimized CC bond lengths, single
and double, were corrected using equations obtained from linear
regression analysis of the data given in Table IX of Ref.[2]. For
the CCl bond, the structure was optimized at the MP2/6-311+G(2d,p)
level and corrected by linear regression analysis of the data given
in Table 4 of Ref.[3]. The CH bond lengths were corrected using
r = 1.001 ropt, where ropt is obtained by MP2/6-31G(d,p)
optimization [4]. Interatomic angles used in the calculation
are those given by MP2/6-311+G(d,p) optimization. |
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Table 2. Z-Matrix (Å and degrees). |
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H |
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C |
1 |
R1 |
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C |
2 |
R2 |
1 |
A3 |
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C |
2 |
R3 |
1 |
A4 |
3 |
180. |
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Cl |
4 |
R4 |
2 |
A5 |
3 |
180. |
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H |
4 |
R5 |
2 |
A6 |
3 |
0. |
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H |
3 |
R6 |
2 |
A7 |
6 |
D1 |
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H |
3 |
R7 |
2 |
A8 |
6 |
-D2 |
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H |
3 |
R7 |
2 |
A8 |
6 |
D2 |
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Conformer I |
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Conformer II |
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R1 |
1.0845 |
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1.084 |
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R2 |
1.4945 |
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1.5035 |
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R3 |
1.329 |
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1.329 |
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R4 |
1.726 |
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1.726 |
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R5 |
1.082 |
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1.082 |
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R6 |
1.090 |
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1.088 |
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R7 |
1.0915 |
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1.091 |
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A3 |
118.28 |
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118.87 |
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A4 |
119.04 |
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118.56 |
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A5 |
123.06 |
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123.00 |
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A6 |
123.36 |
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123.47 |
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A7 |
111.27 |
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110.54 |
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A8 |
110.71 |
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111.45 |
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D1 |
0. |
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180. |
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D2 |
120.40 |
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60.29 |
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[1] R.A.Beaudet, J.Chem.Phys. 37,2398(1962). |
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[2] J.Demaison, J.Cosléou, R.Bocquet,
and A.G.Lesarri, J.Mol.Spectrosc. 167,400(1994). |
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[3] I.Merke, L.Poteau, G.Wlodarczak, A.Bouddou,
and J.Demaison, J.Mol.Spectrosc. 177,232(1996). |
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[4] J.Demaison and G.Wlodarczak, Structural
Chem. 5,57(1994). |
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H2C=CHCl |
H2C=CFCl |
c-ClHC=CHCl
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c-FHC=CHCl |
t-FHC=CHCl |
H2C=CCl2 |
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H2C=CClCN |
F2C=CHCl |
F2C=CCl2 |
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(CH3)2C=CHCl |
Cl2C=CHCl |
F2C=CFCl |
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CH3ClC=CH2 |
c-CH3HC=CHCl |
CH2ClHC=CH2 |
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c-CH3FC=CHCl |
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Table of Contents |
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Molecules/Chlorine |
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t1ClPropene.html |
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Last
Modified 16 June 2004 |
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